Practice #4: defect NST551 TA : Lee Jounghee

Slides:



Advertisements
Similar presentations
Tutorial for Elasticity tool (1) Select (2) Depress For speed, an elastic calculation should be preceded by a careful optimization of atom coordinates.
Advertisements

Research Projects Dr Martin Paul Vaughan available from available from
An ab-initio Study of the Growth and the Field Emission of CNTs : Nitrogen Effect Hyo-Shin Ahn §, Tae-Young Kim §, Seungwu Han †, Doh-Yeon Kim § and Kwang-Ryeol.
DFT – Practice Simple Molecules & Solids [based on Chapters 5 & 2, Sholl & Steckel] Input files Supercells Molecules Solids.
DIAMOND Decommissioning, Immobilisation and Management of Nuclear Wastes for Disposal Density Functional Theory study of defects in zirconolite Jack Mulroue.
Introduction to Solids. 3 Classes of Solids Amorphous – No long range order Polycrystalline – Order within grains Single Crystal – Regular, repeated pattern.
Nuclear Physics Lesson 13
Computing lattice constant, bulk modulus and equilibrium energies of solids Bulk Si Diamond structure.
Javier Junquera Exercises on basis set generation Increasing the angular flexibility: polarization orbitals.
MASTANI 2014 DAY 2 – exercise 3 scf and band structure calculations for Cu (metal) Madhura Marathe No input files available, but should be generated for.
Network for Computational Nanotechnology (NCN) Purdue, Norfolk State, Northwestern, MIT, Molecular Foundry, UC Berkeley, Univ. of Illinois, UTEP DFT Calculations.
Nuclear notation and Binding energy Contents: Atomic notation Isotopes Whiteboard Binding Energy AMU Making an atom Calculating binding energy Whiteboards.
Goal: Graph quadratic functions in different forms.
The H 2 O molecule: converging the size of the simulation box Objectives - study the convergence of the properties with the size of the unit cell.
Launch SpecE8 and React from GSS. You can use the chemical analyses in a GSS data sheet to set up and run SpecE8 and React calculations. Analysis → Launch…
VIRTUAL NANOLAB BY QUANTUMWISE
- Compute and analyze the band structure of an ionic solid
History of Life: Origins of Life Chapter Age of Earth The earth is about 4.5 billion years old How did we measure that? Radiometric Dating = calculating.
First-principles Investigations on Vacancy of Ge in Strained Condition Jung-Hae Choi, Seung-Cheol Lee, and Kwang-Ryeol Lee Computational Science Center.
The eggbox effect: converging the mesh cutoff Objectives - study the convergence of the energy and the forces with respect to the real space grid.
ISU / DEC 10 TH Joaquin Peralta, Rupa Dumpala, and Scott Broderick.
First Principles Calculation of the Field Emission of Nitrogen/Boron Doped Carbon Nanotubes Hyo-Shin Ahn §, Seungwu Han †, Kwang-Ryeol Lee, Do Yeon Kim.
Calculations of Electronic Structure of Defective ZnO: the impact of Symmetry and Phonons A.V. Sorokin, D. Gryaznov, Yu.F. Zhukovskii, E.A. Kotomin, J.
1 P5-26 Topo·chemical transformations in carbon nanotubes: fracture-induced defect, and ad-dimer welding. S. S. MoliverState University Ulyanovsk, Russia.
Band Structure Engineering of Thermoelectric Materials- GeTe Jing ZhiLiang Nov
ATOMS AND IONS What’s the difference?. Atoms vs. Ions  Atoms  Have no overall charge.  The number of protons equals the number of electrons.  Ions.
Chapter 4 An Introduction to Organic Reactions. 4.1 General Principles of Organic Reactions A.Types of Reactions; The Reaction Equation In an organic.
Topic 5.1 and 5.2 Hess’s Law and Bond Enthalpies.
Warm-up: Why do you think we have to learn about chemistry in a biology class? Biochemistry – the study of chemical processes in living organisms.
2/25/2015PHY 752 Spring Lecture 181 PHY 752 Solid State Physics 11-11:50 AM MWF Olin 107 Plan for Lecture 18: Reading: Chapter 10 in MPM Ingredients.
 Grid – A pattern of horizontal and vertical lines, usually forming squares.
Practice #3: Electronic structure
Tutorial of Practice #4 - Supercell & Defect formation energy -
Tutorial of Practice #3 - DOS, band structure, wave function -
Practice #2: Solid Yong-Hyun Kim NST551.
Computing lattice constant, bulk modulus and equilibrium energies of bulk cubic SrTiO 3 Bulk SrTiO 3 Cubic structure.
Computational Physics (Lecture 24) PHY4370. DFT calculations in action: Strain Tuned Doping and Defects.
Visualizing the results o Require the same input file o Final coordinate:  Required: input, CONTCAR  $contcar.x  $xmakemol –f contcar.xyz o Relaxation.
Practice #2: Solid Yong-Hyun Kim NST551.
The Nudged Elastic Band Method and its Implementation in VASP
NOTE: Ignore all GUI warnings A. AOC for 4f2 Add a Pr atom
Isolated Si atoms.
Band structure of a cubic perovskite oxide:
Band Structure Lab with NEMO5 Yi Shen, Nicolás Esquivel Camacho, Michael Povolotskyi ,and Gerhard Klimeck Approach: The communication between Rappture.
Nuclear notation and Binding energy
Chemical Compounds in Cells
Practice #0: Introduction
Intercepts, Symmetry, Even/Odd and intersections
How to plot the Fermi surface using siesta and wannier90
Tutorial - Practice #2 - QnMSG Yong-Hyun Kim.
PH Scale & Buffers Chapter 2 Biochemistry.
ISOTOPES Isotopes are atoms of the same element that have a different number of neutrons. They differ in mass, but the atom’s chemical behavior are.
Effect of Chemical Functionalization on the Raman and Optical Spectra of Carbon Nanotubes Igor Vasiliev, Department of Physics, New Mexico State University,
Applying Determinants to solve Systems of Equations 2x2 & 3x3
Half Life & Radioactive Decay
ATOMIC STRUCTURE Central cell of the Al-SiO2-nSi atomic structure. This cell is connected to Al atomic planes extending to to the left, and n-Si atomic.
Unit 1: Bond Formation, Breaking & Energy
Objectives Solve quadratic equations by graphing or factoring.
Warm Up Find the x-intercept of each function. 1. f(x) = –3x + 9 3
Isotopes Objectives: 5.2 To identify the advantages & disadvantages of using isotopes in industry, medical science, basic research & in the environment.
Graphs of Equations Objectives: Find intercepts from a Graph
Theory- Si an exploration of what is a bond via charge density.
Metastability of the boron-vacancy complex (C center) in silicon: A hybrid functional study Cecil Ouma and Walter Meyer Department of Physics, University.
Isotopes Objectives: 5.2 To identify the advantages & disadvantages of using isotopes in industry, medical science, basic research & in the environment.
Transverse Electric Fields
How to test a norm-conserving pseudopotential
Ability to attract money: 0.00 Pauling
Graphs of Equations Objectives: Find intercepts from a Graph
Radioactive Decay.
When Electric field is applied to free electrons
Presentation transcript:

Practice #4: defect NST551 TA : Lee Jounghee

Supercell structure 1.To make detect-system, the supercell structure have to be made at first. 2.Modify 'input' file where is in same directory with CONTCAR. 3.Create supercell's atomic coordinate (file 'poscar.xyz') > poscar.x 4.Extend cell size in POSCAR and replace the atomic position part with supercell's atomic coordinate in 'poscar.xyz' and 1 C Super cell size (xyz) supercell size supercell's atomic coordinate

Supercell structure 6x6x1 graphene4x4x4 Si

1.Remove a defect atom for one of the original atoms(C, Si) in supercell structure. Defect system calculation(vacancy) Remove line for a carbon atom from original supercell

1.Substitute a defect atom(N) for one of the original atoms(C, Si) in supercell structure. Defect system calculation (substitutional) Add defect atom term in POSCAR ex) 1 N atom, 71 C atoms Original atomic position Defect atomic position Break symmetry for atomic position when the defect atom is added. ex) 

Defect system calculation N-doped grapheneN-doped Si N

Defect system calculation N-doped grapheneN-doped Si

2.Add pseudo potential part of defect atom in POTCAR (same order in POSCAR file). You can find pseudo potential files of every atoms following directory /users/nst551/build/vasp-potentials/PAW_PBE/ 3.Run scf calculation (get CHGCAR). 4.Run non-scf calculation to plot DOS. Nitrogen's pseudo potential part in POTCAR Defect system calculation (substitutional)

DOS of N doped defect systems graphene Si

Defect formation energy means whether the system with defects is more stable or unstable than the bulk system. Defect formation energy E formation (eV) = E(defect system) – [N bulk  bulk + N defect  defect ] E(defects system) : Total energy of system with defects N bulk : Number of bulk atoms  bulk : chemical potential of bulk atoms N defect : Number of defects  defect : chemical potential of defects E f, N-doped graphene = E(N-doped graphene) – [N C  C + N N 1/2  N 2 ],  defect = 1/2  N 2 E f, N-doped Si = E(N-doped Si) – [N Si  Si + N N 1/2  N 2 ],  defect = 1/2  N 2 E(defect system)  bulk N  defect Defect formation energy N-doped graphene N-doped silicon (units: eV) Defect formation energy

Practice #4 1.Make supercell and defect structures for graphene and Si. 2.Plot DOS and find defect states and find defect formation e nergy for graphene and Si. ( ~11/13)